Size matters in miniaturization and automation – smaller is usually better. Traditional electromagnetic motors have limitations when it comes to shrinking dimensions while maintaining high efficiency and accuracy of motion with minimized energy consumption. Piezo ceramic inertia motors can fill this gap. The Q-Motion dubbed miniature direct drives can be employed in linear positioners, rotary stages, goniometer cradles, and even 6-axis parallel positioners. In addition to inertia motors, there are many other types of piezo motors, including ultrasonic drives and high-force piezo-walk drives.
Stick-slip motors are especially cost-effective and can provide nanometer precision motion if required. They provide the best force/size ratio for smallest dimensions.
A piezoelectric ceramic actuator is preloaded against a moving runner. Controlled by a drive signal with a quasi saw-tooth shape, the actuator expands slowly and contracts rapidly (or in the opposite direction). During the slow expansion, the runner sticks to the coupling element and moves along, while during the rapid contraction, the coupling element slips along the runner, which basically stays in place.
Two different versions were developed optimized either for miniature size, moderate force or compact size and higher force.
1. Tangential Inertia Drive Motor
- Very Small Dimensions
- Simple Mechanics
- To 2 N Holding Force
Mini-Rod piezo inertia drives are based on an actuator moving a small rod – or moving along the rod if the rod is fixed. These motors are more powerful than the tangential drives, with up to 10N pushing/holding force. They can be integrated into linear actuators and linear positioning stages, however the principle does not apply to rotary stages.
The operating principle is shown in the animation.
An application of the Q-545.140 closed-loop servo linear stages in high resolution interferometry used for quantum information processing is described in this paper “Temporal-mode-selective optical Ramsey interferometry via cascaded frequency conversion” that deals with storage and retrieval of quantum information, written by Dileep V. Reddy and Michael G. Raymer, Oregon Center for Molecular, Optical and Quantum Science and Department of Physics, University of Oregon, Eugene, Oregon USA.
The nanopositioning stages used provide an encoder-based position read-out precision of 1nm.
During the stick phase, the runner is moved in the defined direction.
During the slip phase, the runner does not move. The so-called back-stepping effect leads to a small backward motion during the acceleration phase of the piezo actuator.
The typical feed- motion per full cycle is 300 nm to 1 µm. It depends on the actuator type and force acting on the actuator.
The actuator can be controlled to any position within its range with sub-nm resolution by changing the drive voltage (analog mode).
Self-Locking at Rest
As with most piezo motors, Q-Motion inertia drives are self-locking at rest. There is no power consumption, no heat dissipation, no position dither.
Between each stick and slip cycle, a miniscule position shift called the back-stepping effect can be noticed. This effect is inseparably connected with the inertia drive principle and its relevance depends on the application.
At a data sample rate of 133 kHz, a backstepping effect is too small to be noticed! Consequentially, we state that the backstepping effect does not influence the constancy and smoothness of velocity. However, there are other factors that directly influence the velocity.
Constancy of Velocity at a Microscopic Level
With the entry level E-871.1A1 motion controller, the selected velocity is reached by adjusting the operating frequency. Adjusting the frequency means that the voltage profile of a single step remains constant with pauses in between. The E-873 controller offers more sophisticated velocity control.
Other Piezo Motor Drives
Comparison of different piezo motors
Lifetime is affected by load, duty cycle, environmental conditions (humidity, vacuum), etc., based on wear motion ranges of >20km are feasible.
Ideal applications demand:
- Duty cycles below 50 %
- Continuous operating time <10 sec (2x back and forth across the complete travel range)
6-Axis Parallel Positioners
In addition to linear and rotary positioners, linear stages can be combined to 6-axis parallel arrangements.
The E-873 3-channel motion controller features:
- Broadband encoder input
- Macro programmable for stand-alone functionality
- Data recorder
- Nonvolatile EEPROM for macros and parameters
- Digital I/O ports (TTL)
- ID chip support
- Interfaces: TCP/IP and USB
- Optional digital joystick for manual operation a single channnel version is available as the E-871
- For PIShift and PiezoMike Piezo Inertia Drives
- Ideal for OEM Applications
- One to Four Actuators, Serial Control (through demultiplexing)
- With Digital USB interface
- Host Software LabVIEW Driver Included
Features of the E-872.01 and E-472.02 OEM driver include:
- Step-Direction Input Signal
- E-872.01: Full Step Modus
- E-872.02: Micro Step Modus
- Cost Effective
The E-873 Macro programmable specifications include:
- Data Recorder
- Digital I/ O Ports (TTL)
- ID Chip Support
- Interfaces: USB, RS-232 and TCP/ IP
- Joystick Input for Manual Operation
- Velocity Control
- Compatible Sub-D Connectors for Q-Motion Stages
- Optionally Available with Metal-Sheet Housing for OEM Applications
Vacuum and Nonmagnetic Operation
High-Vacuum to 10-6 hPa
Standard and unprepared Q-Motion stages can be used in ambient conditions and for vacuum up to 10-6 hPa. For vacuum operation, the C-815.VF vacuum feedthrough is available.
On the air side, the following cables will be available for connecting the feedthrough with the controller E-873 (plus adapter cable for E-871, which is included in the delivery of the stage):
These air-side cables also work for the feedthrough for UHV.
Ultrahigh Vacuum to 10-9 hPa
Ultrahigh vacuum models are also available.
PI is currently evaluating ceramic bearings for nonmagnetic stage designs. Nonmagnetic operation is of interest in the environment of electron beam imaging such as lithography or microscopy.
Tests in high magnetic fields
The KIT (Karlsruhe Institute of Technology) has performed tests in high magnetic fields of 9.4 Tesla (T). The stage (not operating) was not attracted by the magnetic field and was not magnetized.
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